표 2. | Table. 2. V_in가 주어져 있으며, l ≠ 0일 때, 각 전원들의 수식 | Source equations when V_in is given with l ≠ 0.

Vin	Incident wave	Reflected wave	Input wave (total wave)
Voltage @z=−l	V i n c   = V + ( z = − l ) = V i n 1 + Γ L e − 2 j β l	V r e f l e c t e d   = V − ( z = − l ) = V i n ( 1 + Γ L e − 2 j β l ) Γ L e − 2 j β l	Vin
Current @z=−l	I i n c = I + ( z = − l ) = V i n Z 0 ⋅ ( 1 + Γ L e − 2 j β l )	I r e f l e c t e d   = I − ( z = − l ) = − V i n Z 0 ⋅ ( 1 + Γ L e − 2 j β l ) Γ L e − 2 j β l	I i n = I + ( z = − l ) + I − ( z = − l ) = V i n Z 0 ⋅ 1 − Γ L e − 2 j β l 1 + Γ L e − 2 j β l
Power @z=−l	P i n c = 1 2 R e ( V i n c ⋅ I i n c * ) = 1 2 R e ( V i n 1 + Γ L e − 2 j β l ⋅ ( V i n Z 0 ⋅ ( 1 + Γ L e − 2 j β l ) ) * ) = | V i n | 2 2 Z 0 1 | 1 + Γ L e − 2 j β l | 2	P r e f l e c t e d   = 1 2 R e ( V r e f l e c t e d   ⋅ I r e f l e c t e d   * ) = 1 2 R e ( V i n ( 1 + Γ L e − 2 j β l ) Γ L e − 2 j β l ⋅ ( V i n ) * Z 0 ⋅ ( 1 + Γ L . e 2 j β l ) Γ L * e 2 j β l ) = − | V i n | 2 2 Z 0 ⋅ | Γ L | 2 | 1 + Γ L e − 2 j β l | 2	P i n   = 1 2 R e ( V i n ⋅ I i n * ) = | V i n | 2 2 Z 0 R e ( ( 1 + Γ L e − 2 j β l ) ( 1 + Γ L e − 2 j β l ) ⋅ ( 1 − Γ L e − 2 j β l ) * ( 1 + Γ L e − 2 j β l ) * ) = | V i n | 2 2 Z 0 ⋅ 1 − | Γ L | 2 | 1 + Γ L e − 2 j β l | 2